System and method of aligning scintillator crystalline structures for computed tomography imaging

ABSTRACT

The present invention discloses a method of aligning scintillator crystalline structures for computed tomography imaging and a system of use. Crystal seeds are deposited inside a glass melt and are then grown to form a plurality of layer crystallites. While growing the crystallites, a field is applied to align each crystallite structure in a uniform orientation. As a result, the crystallites are configured to reduce light scattering and improve the overall efficiency of the CT system. A CT system is disclosed implementing a scintillator array having a plurality of scintillators, each scintillator being formed of a plurality of uniformly aligned crystallites. Each crystallite includes a receiving surface and an exiting surface configured perpendicular to an x-ray beam. Further, the receiving surface and the exiting surface are connected by a plurality of surface walls arranged parallel to the x-ray beam.

BACKGROUND OF INVENTION

[0001] The present invention relates generally to the detection andconversion of high frequency electromagnetic energy to electricalsignals and, more particularly, to a method of aligning scintillatorcrystalline structures and a system of use.

[0002] Typically, in computed tomography (CT) imaging systems, an x-raysource emits a fan-shaped beam toward an object, such as a patient. Thebeam, after being attenuated by the object, impinges upon an array ofradiation detectors. The intensity of the attenuated beam of radiationreceived at the detector array is typically dependent upon theattenuation of the x-ray beam by the object. Each detector element ofthe detector array produces a separate electrical signal indicative ofthe attenuated beam received by each detector element. The electricalsignals are transmitted to a data processing system for analysis whichultimately results in the formation of an image.

[0003] Generally, the x-ray source and the detector array are rotatedabout the gantry within an imaging plane and around the object. X-raysources typically include x-ray tubes, which emit the x-ray beam at afocal point. X-ray detectors typically include a collimator forcollimating x-ray beams received at the detector, a scintillator forconverting x-rays to light energy adjacent the collimator, andphotodiodes for receiving the light energy from the adjacentscintillator.

[0004] Typically, a ceramic scintillator of a CT system is formed by alarge number of small crystalline structures or crystallites. Thechemical compound used to form the scintillator material generallydefines a particular crystalline structure or geometrical shape of eachcrystallite. Regardless of geometrical shape, in some knownscintillators, the crystallites are not optimally aligned. In theseknown scintillators, the orientation of the crystallites is notsufficiently controlled thereby increasing light scattering. Moreover,in known CT systems, the light receiving surface of each crystallite isnot parallel to the structure's light exiting surface, therebyincreasing light scattering further and decreasing the overallefficiency of the scintillator detector and the CT system.

[0005] It would therefore be desirable to design a scintillator withproperly aligned and orientated crystallites that reduces lightscattering and improves detector and CT system efficiency.

BRIEF DESCRIPTION OF INVENTION

[0006] The present invention provides a detector for a CT system thatovercomes the aforementioned drawbacks. The detector includes ascintillator for receiving and converting high frequency electromagneticenergy to light energy. The scintillator includes a plurality ofcrystallites that are aligned parallel to a high frequencyelectromagnetic energy beam. Properly aligning the crystallites of thescintillator improves the efficiency of the CT system.

[0007] In accordance with one aspect of the invention, a method fororientating crystallites in CT scintillators is provided. The methodincludes melting a composition configured to convert high frequencyelectromagnetic energy to light energy into a glass melt. The glass meltis then shaped into one of a number of geometrical configurationsdepending upon the particular CT system. After shaping the glass melt,crystal seeds are deposited inside the glass melt. The method furtherincludes growing crystallites in the glass melt from the crystal seedsand applying a field to the glass melt while growing the crystallites.

[0008] In accordance with another aspect of the invention, a method ofCT imaging includes providing a plurality of scintillators forming ascintillator array wherein each scintillator includes a plurality ofcrystallites. The method further includes the step of aligning thecrystallites of each scintillator in a uniform direction to receive highfrequency electromagnetic energy from a projection source. Theprojection source directs high frequency electromagnetic energy towardthe scintillator array wherein the high frequency electromagnetic energyis converted to light energy. The method also includes transmittingsignals indicative of light energy intensity to a data acquisitionsystem and generating a CT image from the transmitted signals.

[0009] In accordance with yet another aspect of the invention, a CTsystem implementing a plurality of scintillators having a plurality ofuniformly aligned crystallites-is provided. The system has a highfrequency electromagnetic energy projection source configured to projecta high frequency electromagnetic energy beam toward the plurality ofscintillators. A photodiode array having a plurality of photodiodes andoptically coupled to the plurality of scintillators is provided toreceive light energy output from the plurality of scintillators. Thesystem further includes a gantry having an opening to receive a subjectobject.

[0010] Various other features, objects and advantages of the presentinvention will be made apparent from the following detailed descriptionand the drawings.

BRIEF DESCRIPTION OF DRAWINGS

[0011] The drawings illustrate one preferred embodiment presentlycontemplated for carrying out the invention.

[0012] In the drawings:

[0013]FIG. 1 is a pictorial view of a CT imaging system;

[0014]FIG. 2 is a block schematic diagram of the system illustrated inFIG. 1;

[0015]FIG. 3 is a perspective view of one embodiment of a CT systemdetector array;

[0016]FIG. 4 is a perspective view of one embodiment of a detector;

[0017]FIG. 5 is illustrative of various configurations of the detectorin FIG. 4 in a four-slice mode; and

[0018]FIG. 6 is a perspective view of a crystallite according to oneembodiment of the present invention.

DETAILED DESCRIPTION

[0019] The operating environment of the present invention is describedwith respect to a four-slice computed tomography (CT) system. However,it will be appreciated by those of ordinary skill in the art that thepresent invention is equally applicable for use with single-slice orother multi-slice configurations. Moreover, the present invention willbe described with respect to the detection and conversion of x-rays.However, one of ordinary skill in the art will further appreciate, thatthe present invention is equally applicable for the detection andconversion of other high frequency electromagnetic energy.

[0020] Referring to FIGS. 1 and 2, a computed tomography (CT) imagingsystem 10 is shown as including a gantry 12 representative of a “thirdgeneration” CT scanner. Gantry 12 has an x-ray source 14 that projects abeam of x-rays 16 toward a detector array 18 on the opposite side of thegantry 12. Detector array 18 is formed by a plurality of detectors 20which together sense the projected x-rays that pass through a medicalpatient 22. Each detector 20 produces an electrical signal thatrepresents the intensity of an impinging x-ray beam and hence theattenuated beam as it passes through the patient 22. During a scan toacquire x-ray projection data, gantry 12 and the components mountedthereon rotate about a center of rotation 24.

[0021] Rotation of gantry 12 and the operation of x-ray source 14 aregoverned by a control mechanism 26 of CT system 10. Control mechanism 26includes an x-ray controller 28 that provides power and timing signalsto an x-ray source 14 and a gantry motor controller 30 that controls therotational speed and position of gantry 12. A data acquisition system(DAS) 32 in control mechanism 26 samples analog data from detectors 20and converts the data to digital signals for subsequent processing.

[0022] An image reconstructor 34 receives sampled and digitized x-raydata from DAS 32 and performs high speed reconstruction. Thereconstructed image is applied as an input to a computer 36 which storesthe image in a mass storage device 38.

[0023] Computer 36 also receives commands and scanning parameters froman operator via console 40 that has a keyboard. An associated cathoderay tube display 42 allows the operator to observe the reconstructedimage and other data from computer 36.

[0024] The operator supplied commands and parameters are used bycomputer 36 to provide control signals and information to DAS 32, x-raycontroller 28 and gantry motor controller 30. In addition, computer 36operates a table motor controller 44 which controls a motorized table 46to position patient 22 and gantry 12. Particularly, table 46 movesportions of patient 22 through a gantry opening 48.

[0025] As shown in FIGS. 3 and 4, detector array 18 includes a pluralityof scintillators 57 forming a scintillator array 56. A collimator (notshown) is positioned above scintillator array 56 to collimate x-raybeams 16 before such beams impinge upon scintillator array 56.

[0026] In one embodiment, shown in FIG. 3, detector array 18 includes 57detectors 20, each detector 20 having an array size of 16×16. As aresult, array 18 has 16 rows and 912 columns (16×57 detectors) whichallows 16 simultaneous slices of data to be collected with each rotationof gantry 12.

[0027] Switch arrays 80 and 82, FIG. 4, are multi-dimensionalsemiconductor arrays coupled between scintillator array 56 and DAS 32.Switch arrays 80 and 82 include a plurality of field effect transistors(FET) (not shown) arranged as multi-dimensional array. The FET arrayincludes a number of electrical leads connected to each of therespective scintillators and a number of output leads electricallyconnected to DAS 32 via a flexible electrical interface 84.Particularly, about one-half of scintillator outputs are electricallyconnected to switch 80 with the other one-half of scintillator outputselectrically connected to switch 82. Each detector 20 is secured to adetector frame 77, FIG. 3, by mounting brackets 79.

[0028] Switch arrays 80 and 82 further include a decoder (not shown)that control enables, disables, or combines scintillator outputs inaccordance with a desired number of slices and slice resolutions foreach slice. Decoder, in one embodiment, is a decoder chip or a FETcontroller as known in the art. Decoder includes a plurality of outputand control lines coupled to switch arrays 80 and 82 and DAS 32. In oneembodiment defined as a 16 slice mode, decoder enables switch arrays 80and 82 so that all rows of the scintillator array 52 are activated,resulting in 16 simultaneous slices of data for processing by DAS 32. Ofcourse, many other slice combinations are possible. For example, decodermay also select from other slice modes, including one, two, andfour-slice modes.

[0029] As shown in FIG. 5, by transmitting the appropriate decoderinstructions, switch arrays 80 and 82 can be configured in thefour-slice mode so that the data is collected from four slices of one ormore rows of scintillator array 56. Depending upon the specificconfiguration of switch arrays 80 and 82, various combinations ofscintillators 57 can be enabled, disabled, or combined so that the slicethickness may consist of one, two, three, or four rows of scintillatorarray elements 57. Additional examples include, a single slice modeincluding one slice with slices ranging from 1.25 mm thick to 20 mmthick, and a two slice mode including two slices with slices rangingfrom 1.25 mm thick to 10 mm thick. Additional modes beyond thosedescribed are contemplated.

[0030] Now referring to FIG. 6, and in a preferred embodiment, eachscintillator comprises a plurality of crystallites 90. The presentinvention will be described with respect to the hexagonal crystallinestructure 90 shown in FIG. 6, however, one of ordinary skill in the artwill appreciate that the present invention is equally applicable toother polygonal crystalline structures. Each crystallite 90 includes areceiving surface 92 and a exiting surface 94. In the hexagonalcrystalline structure 90 shown, six surface walls generally designated96 are provided connecting the receiving surface 92 and the exitingsurface 94. As shown, the surface walls 96 are configured perpendicularat approximately 90° to both the receiving surface 92 and the exitingsurface 94. By configuring the surface walls 96 perpendicularly to thereceiving surface 92 and the exiting surface 94, the receiving surface92 and the exiting surface 94 are arranged parallel to one another alonga constant plane. Furthermore, the receiving surface 92 and the exitingsurface 94 are configured perpendicular to beam of x-rays 16 and thesurface walls 96 are arranged parallel to the beam of x-rays 16.Orientating receiving surface 92 and exiting surface 94 perpendicular tox-ray beam 16 and orientating surface walls 96 parallel to x-ray beam16, light scattering in the scintillator is reduced while increasing theoverall efficiency of the scintillator and CT system.

[0031] Accordingly, the present invention contemplates a method ofaligning scintillator crystallites for a computed tomography imagingsystem. The method includes melting a composition configured to converthigh frequency electromagnetic energy to light energy, and in apreferred embodiment, into a glass melt. The glass melt is thenconfigured into one of a number forms, such as, a layered form, alaminated form, or a columnated form. Crystal seeds, a few nanometers insize, are then deposited inside the glass melt and grown to form acrystalline phase. The growing crystallites will share the samepolygonal structure, but will not be uniformly aligned. As a result, themethod includes the step of applying a field to the glass melt whilegrowing the crystallites. In one preferred embodiment, the field is anelectric field wherein a bias voltage is applied across the glass melt.The electric field applied across the glass melt will align thecrystallites in a uniform direction. This is achieved because eachcrystallite of the glass melt has a dipole moment, therefore, onesurface 92, 94 will orientate with the positive voltage and the othersurface 94, 92 will align with the negative voltage. As the crystallitesare grown, each new crystallite structure will be properly orientateduntil each crystallite structure is formed and the bulk material willbecome a glass ceramic. The electric field will be maintained across theglass ceramic after the growing phase ceases and subsequent cooling ofthe glass ceramic. When the glass ceramic has cooled, the electric fieldis removed and a uniformly aligned and properly orientated scintillatorresults.

[0032] Alternatively, the crystallites may be uniformly aligned andorientated by applying a magnetic field, an electromagnetic field, anoptical field, a thermal field, or a mechanical stress to the glassmelt.

[0033] The present invention further includes a method of CT imagingincluding the steps of providing a plurality of scintillators forming ascintillator array wherein each scintillator includes a plurality ofcrystallites. The crystallites are then aligned in a uniform directionto receive high frequency electromagnetic energy from a projectionsource. In a preferred embodiment, the high frequency electromagneticenergy is x-ray energy, but the instant invention is applicable withother forms of high frequency electromagnetic energy. The high frequencyelectromagnetic energy directed toward the scintillator array isreceived and converted to light energy. In a preferred embodiment, aphotodiode array comprising a plurality of photodiodes and opticallycoupled to the scintillator array detects the light energy emitted byeach scintillator of the scintillator array and transmits signalsindicative of light energy intensity to a data acquisition systemwhereupon the signals are analyzed and a CT image is generated.

[0034] The present invention further includes a CT system that has aplurality of scintillators including a plurality of uniformly alignedcrystallites. A high frequency electromagnetic energy projection sourceis configured to project a high frequency electromagnetic energy beamtoward the plurality of scintillators. In a preferred embodiment, thehigh frequency electromagnetic energy beam is an x-ray beam. The systemfurther includes a photodiode array having a plurality of photodiodesoptically coupled to the plurality of scintillators to receive lightenergy output therefrom and a gantry having an opening to receive asubject object, such as a medical patient.

[0035] Each uniformly aligned crystallite of each scintillator includesa receiving surface, an exiting surface, and a plurality of surfacewalls connecting the receiving surface and the exiting surface. In thehexagonal crystalline structure shown in FIG. 6, six surface wallsconnect the receiving and exiting surfaces. However, the instantinvention is further applicable to other polygonal crystallinestructures. Regardless of the particular polygonal crystallinestructure, each surface wall is configured perpendicularly to thereceiving surface and the exiting surface. As a result, the receivingsurface and the exiting surface are co-planar and are configuredperpendicularly to the high frequency electromagnetic energy beam.Moreover, the plurality of surface walls are configured parallel to thehigh frequency electromagnetic energy beam.

[0036] The present invention has been described in terms of thepreferred embodiment, and it is recognized that equivalents,alternatives, and modifications, aside from those expressly stated, arepossible and within the scope of the appending claims.

What is claimed is:
 1. A method for orientating crystallites in CTscintillators comprising the steps of: melting a composition configuredto convert high frequency electromagnetic energy to light energy into aglass melt; shaping the glass melt; depositing crystal seeds inside theglass melt; growing crystallites in the glass melt from the crystalseeds; and applying a field to the glass melt while growing thecrystallites.
 2. The method of claim 1 further comprising the step ofaligning the crystallites in a uniform orientation.
 3. The method ofclaim 1 wherein the step of applying a field includes applying one of anelectric field, a magnetic field, an electromagnetic field, an opticalfield, a thermal field, and a mechanical stress.
 4. The method of claim2 further comprising the step of configuring the crystallites parallelto a high frequency electromagnetic energy path.
 5. The method of claim1 wherein the step of shaping includes one of layering, laminating, andcolumnating the glass melt.
 6. A method of CT imaging comprising thesteps of: providing a plurality of scintillators forming a scintillatorarray wherein each scintillator comprises a plurality of crystallites;aligning the crystallites of each scintillator in a uniform direction toreceive high frequency electromagnetic energy from a projection source;directing high frequency electromagnetic energy toward the scintillatorarray; converting the high frequency electromagnetic energy to lightenergy; transmitting signals indicative of light energy intensity to adata acquisition system; and generating a CT image from the transmittedsignals.
 7. The method of claim 6 wherein the step of aligning furtherincludes the step of configuring the crystallites parallel to a path ofhigh frequency electromagnetic energy projection.
 8. The method of claim6 wherein the step of providing a plurality of scintillators furtherincludes the step of precipitating nuclei into a glass melt to form theplurality of crystallites.
 9. The method of claim 8 further comprisingthe step of growing the crystallites from the precipitated nuclei. 10.The method of claim 9 further comprising the step of crystallizing theglass melt and enlarging the precipitated nuclei to form a crystallinephase.
 11. The method of claim 10 further comprising the step ofapplying one of an electric field and a magnetic field across the glassmelt during the crystallization step.
 12. The method of claim 11 furthercomprising the step of applying the electric field to a ferroelectriccrystalline phase and the magnetic field to a ferromagnetic crystallinephase.
 13. The method of claim 6 further comprising the step ofimproving light collecting efficiency of the scintillators.
 14. Themethod of claim 6 further comprising the step of eliminating externallight cladding.
 15. The method of claim 6 wherein each of the pluralityof crystallites have polygonal crystalline structures.
 16. The method ofclaim 6 wherein each of the plurality of crystallites have a hexagonalcrystalline structure.
 17. A CT system comprising: a plurality ofscintillators including a plurality of uniformly aligned crystallites; ahigh frequency electromagnetic energy projection source configured toproject a high frequency electromagnetic energy beam toward theplurality of scintillators; a photodiode array having a plurality ofphotodiodes optically coupled to the plurality of scintillators toreceive light energy output therefrom; and a gantry having an opening toreceive a subject to be scanned.
 18. The CT system of claim 17 whereineach uniformly aligned crystalline structure includes a receivingsurface, an exiting surface, and a plurality of surface walls connectingthe receiving surface and the exiting surface, wherein the receivingsurface and the exiting surface are coplanar.
 19. The CT system of claim18 wherein each surface wall is configured perpendicularly to thereceiving surface and the exiting surface.
 20. The CT system of claim 18wherein the receiving surface and the exiting surface are configuredperpendicularly to the high frequency electromagnetic energy beam andthe plurality of surface walls are configured parallel to the highfrequency electromagnetic energy beam.
 21. The CT system of claim 17wherein the at least one scintillator is a glass ceramic.
 22. The CTsystem of claim 17 wherein the plurality of scintillators produce lightenergy having an intensity indicative of high frequency electromagneticenergy beam attenuation by the subject.
 23. The CT system of claim 17wherein the subject is a patient and the high frequency electromagneticbeam is an x-ray beam.
 24. The CT system of claim 17 wherein each of theplurality of uniformly aligned crystallite have a polygonal crystallinestructure.
 25. The CT system of claim 17 wherein each of the pluralityof uniformly aligned crystallites has a hexagonal crystalline structure.